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Search Results (3,108)

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Keywords = resistive sensor

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14 pages, 4126 KiB  
Article
Real-Time Respiratory Monitoring Using a Sparse-Sampled Frequency-Scanning White-Light Interferometry System
by Wenyan Liu, Cheng Qian, Kexin Li, Yiping Wang, Xiaoyan Cai and Qiang Liu
Photonics 2025, 12(1), 45; https://doi.org/10.3390/photonics12010045 - 6 Jan 2025
Abstract
Fiber-optic tip sensors offer significant potential in biomedical applications due to their high sensitivity, compact size, and resistance to electromagnetic interference. This study focuses on advancing phase demodulation techniques for ultra-short Fabry–Pérot cavities within limited spectral bandwidths to enhance their application in biomedicine [...] Read more.
Fiber-optic tip sensors offer significant potential in biomedical applications due to their high sensitivity, compact size, and resistance to electromagnetic interference. This study focuses on advancing phase demodulation techniques for ultra-short Fabry–Pérot cavities within limited spectral bandwidths to enhance their application in biomedicine and diagnostics. We propose a novel sparse-sampled white-light interferometry system for respiratory monitoring, utilizing a monolithic integrated semiconductor tunable laser for quasi-continuous frequency scanning across 191.2–196.15 THz at a sampling rate of 5 kHz. A four-step phase-shifting algorithm (PSA) ensures precise phase demodulation, enabling high sensitivity for short-cavity fiber-optic sensors under constrained spectral bandwidth conditions. Humidity sensors fabricated via a self-growing polymerization process further enhance the system’s functionality. The experimental results demonstrate the system’s capability to accurately capture diverse breathing patterns—including normal, rapid, and deep states—with fast response and recovery times. These findings establish the system’s potential for real-time respiratory monitoring in clinical and point-of-care settings. Full article
(This article belongs to the Special Issue Advancements in Optical Fiber Sensing)
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<p>Sparse-sampled frequency-scanning white-light interferometry system. (<b>a</b>) Block diagram of the driver and data acquisition module of the MG-Y laser. (<b>b</b>) Pictures of key modules. 1, FPGA; 2, analog-to-digital conversion module; 3, driver board for current sources; 4, photodetectors; 5, MG-Y laser.</p>
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<p>Current tuning curves of sparsely sampled optical frequency scanning process.</p>
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<p>Schematic diagram of the sensor fabrication process. (<b>a</b>–<b>c</b>) Adsorption of photopolymer droplet film on optical fiber end face; (<b>d</b>) self-growing polymerization based on a 520 nm green laser; (<b>e</b>) microscopic image of a fiber tip humidity sensor.</p>
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<p>Principle of four-step phase-shifting demodulation scheme. (<b>a</b>) Sparsely sampled initial interferometer spectrum; (<b>b</b>) phase-shifted spectrum after splitting.</p>
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<p>Simulated demodulation results of a 50 Hz, 600 nm peak-to-peak amplitude sinusoidal vibration. (<b>a</b>) Interference spectra at different times; (<b>b</b>) comparison of demodulation results and theoretical values.</p>
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<p>Graph of RMSE simulation results for measuring sinusoidal dynamic signals.</p>
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<p>Schematic diagram of the proposed system and conventional WLI system for vibration measurement.</p>
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<p>Vibration measurement results. (<b>a</b>) Spectrum collected by the proposed system; (<b>b</b>) spectrum collected by conventional broadband WLI; (<b>c</b>) comparison of demodulation results between the two systems.</p>
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<p>Experimental results of relative humidity detection. (<b>a</b>) The measured reflected spectra evolution with increasing humidity; (<b>b</b>) the ΔOPD at different humidities and the linear fitting results.</p>
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<p>Compact fiber-optic respiratory monitoring system. The red rectangle marks the fiber tip sensor.</p>
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<p>Time-domain response curves of different breathing states. (<b>a</b>) Normal breathing; (<b>b</b>) enlarged view of one breathing process; (<b>c</b>) fast breathing; (<b>d</b>) deep breathing.</p>
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21 pages, 23995 KiB  
Article
A Hybrid Dual-Axis Solar Tracking System: Combining Light-Sensing and Time-Based GPS for Optimal Energy Efficiency
by Muhammad Hammas, Hassen Fituri, Ali Shour, Ashraf Ali Khan, Usman Ali Khan and Shehab Ahmed
Energies 2025, 18(1), 217; https://doi.org/10.3390/en18010217 - 6 Jan 2025
Abstract
Fixed solar panels face significant energy loss as they cannot consistently capture optimal sunlight. Because of that, the overall efficiency of the PV panel will be reduced, and the installation requires larger land space to generate appropriate power; this stems from the use [...] Read more.
Fixed solar panels face significant energy loss as they cannot consistently capture optimal sunlight. Because of that, the overall efficiency of the PV panel will be reduced, and the installation requires larger land space to generate appropriate power; this stems from the use of a dual-axis solar tracking system, which can significantly increase overall energy production. The system is based on the combination of two approaches to precisely track the sunlight: first, using multiple LDRs (light-dependent resistors) as photo sensors to track the position of the sun by balancing the resistivity using a proportional integral deprival (PID) controller, and the second approach using the time-based control for cloudy days when sunlight is diffused, getting the time GPS coordinates and time to calculate the accurate position of the sun by determining the azimuth and altitude angle. This dual system significantly improves energy production by 33.23% compared to fixed systems and eliminates errors during shaded conditions while reducing unnecessary energy use from continuous GPS activation. The prototype uses two linear actuators for both angles and a 100-watt solar panel mounted on the dual-axis platform. Full article
(This article belongs to the Special Issue Power Quality and Hosting Capacity in the Microgrids)
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<p>Block diagram illustrating the proposed hybrid dual-axis solar tracking system, combining real-time sunlight sensing with time-based GPS tracking for optimized solar energy capture.</p>
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<p>Electrical circuit diagram of the dual-axis solar tracking system showing connections between sensors, controllers, and actuators.</p>
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<p>Mechanical structure of the dual-axis solar tracking system, highlighting the two pivot points for azimuth and altitude adjustments, supported by linear actuators.</p>
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<p>Equivalent circuit model of a single photovoltaic (PV) cell used for energy generation, depicting the relationship between the current, voltage, and resistance.</p>
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<p>Annual sun path diagram showing the azimuth and tilt angles used for designing the dual-axis tracking system to optimize solar exposure.</p>
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<p>Illustration of the solar panel’s angular adjustments enabled by linear actuators for azimuth and tilt tracking based on light intensity changes.</p>
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<p>Effect of sunlight on light-dependent resistors (LDRs) under varying conditions: (<b>A</b>) sunlight concentration on the south LDR, (<b>B</b>) balanced sunlight concentration across all LDRs, and (<b>C</b>) sunlight concentration on the east LDR.</p>
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<p>Schematic diagram of the light sensor module, showing the connection of LDRs to the microcontroller using pull-down resistors for accurate light-intensity measurement.</p>
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<p>Flow diagram of the solar tracking algorithm, illustrating the decision-making processes for adjusting the azimuth and tilt angles based on light intensity and time-based control.</p>
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<p>Block diagram of the PID control system for regulating linear actuator movements to ensure precise solar panel tracking.</p>
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<p>Internal model control (IMC)-based PID control block diagram for optimizing solar tracking performance, showing control-loop feedback mechanisms.</p>
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<p>Daily solar path for St. John’s, NL, illustrating changes in azimuth and altitude angles from sunrise to sunset for optimizing panel positioning.</p>
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<p>Flow diagram of the IoT-based data acquisition system for real-time monitoring of GPS coordinates and solar power output.</p>
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<p>The change in the analog reading values of all LDR sensors.</p>
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<p>Assembled prototype with component labeling.</p>
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<p>Current of the PV panel at a fixed position of <math display="inline"><semantics> <msup> <mn>30</mn> <mo>∘</mo> </msup> </semantics></math> latitude.</p>
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<p>Voltage of the PV panel at a fixed position of <math display="inline"><semantics> <msup> <mn>30</mn> <mo>∘</mo> </msup> </semantics></math> latitude.</p>
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<p>Power of the PV panel at a fixed position of <math display="inline"><semantics> <msup> <mn>30</mn> <mo>∘</mo> </msup> </semantics></math> latitude.</p>
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<p>Voltage and current of the PV panel using the solar tracking system.</p>
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<p>Power of the PV panel using a solar tracking system.</p>
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<p>The difference in the power of both systems.</p>
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10 pages, 3446 KiB  
Communication
High-Temporal-Resolution Corrosion Monitoring in Fluctuating-Temperature Environments with an Improved Electrical Resistance Sensor
by Mao Takeyama
Sensors 2025, 25(1), 268; https://doi.org/10.3390/s25010268 - 6 Jan 2025
Viewed by 110
Abstract
The electrical resistance (ER) method is widely used for atmospheric corrosion measurements and can be used to measure the corrosion rate accurately. However, severe errors occur in environments with temperature fluctuations, such as areas exposed to solar radiation, preventing accurate temporal corrosion rate [...] Read more.
The electrical resistance (ER) method is widely used for atmospheric corrosion measurements and can be used to measure the corrosion rate accurately. However, severe errors occur in environments with temperature fluctuations, such as areas exposed to solar radiation, preventing accurate temporal corrosion rate measurement. To decrease the error, we developed an improved sensor composed of a reference metal film and an overlaid sensor metal film to cancel temperature differences between them. The improved sensor was compared with an existing sensor product in outdoor monitoring experiments. The spike-like error during the daytime was successfully reduced. Furthermore, by utilizing a data-filtering process, we measured the corrosion rate every hour. Hourly corrosion rate measurements were difficult when the average daily corrosion rate was less than 50 µm/year under conditions of 0.05 g/m2 salt. Observations showed a strong correlation between corrosion rate and sensor surface humidity. In the future, this method will make it possible to study the relationship between the atmospheric corrosion rate and environmental changes over time. Full article
(This article belongs to the Special Issue Novel Sensing Technologies for Environmental Monitoring and Detection)
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<p>Design of improved ER sensor. Right is the top view and left is the side view.</p>
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<p>Picture of the improved sensor (<b>left</b>) and existing product (<b>right</b>). Thermocouples were attached to the surface of the existing product.</p>
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<p>Time series data of observations. From top to bottom: corrosion depth measured with existing products, temperature, humidity, solar radiation, corrosion depth compensated for with surface temperature, and corrosion depth measured with improved sensors.</p>
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<p>Comparison of measured daily corrosion depths between product and improved sensors.</p>
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<p>Detailed corrosion depth for one day: raw data and linear approximation after data processing.</p>
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<p>Histograms of residuals for correct period and error period.</p>
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<p>Time series of corrosion depth, corrosion rate, and relative humidity.</p>
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16 pages, 13181 KiB  
Article
An Open-Source 3D Printed Three-Fingered Robotic Gripper for Adaptable and Effective Grasping
by Francisco Yumbla, Emiliano Quinones Yumbla, Erick Mendoza, Cristobal Lara, Javier Pagalo, Efraín Terán, Redhwan Algabri, Myeongyun Doh, Tuan Luong and Hyungpil Moon
Biomimetics 2025, 10(1), 26; https://doi.org/10.3390/biomimetics10010026 - 4 Jan 2025
Viewed by 259
Abstract
This research focuses on the design of a three-finger adaptive gripper using additive manufacturing and electromechanical actuators, with the purpose of providing a low-cost, efficient, and reliable solution for easy integration with any robot arm for industrial and research purposes. During the development [...] Read more.
This research focuses on the design of a three-finger adaptive gripper using additive manufacturing and electromechanical actuators, with the purpose of providing a low-cost, efficient, and reliable solution for easy integration with any robot arm for industrial and research purposes. During the development phase, 3D printing materials were employed in the gripper’s design, with Polylactic Acid (PLA) filament used for the rigid mechanical components and Thermoplastic Polyurethane (TPU) for the flexible membranes that distribute pressure to the resistive force sensors. Stress analysis and simulations were conducted to evaluate the performance of the components under load and to gradually refine the design of the adaptive gripper. It was ensured that the mechanism could integrate effectively with the robotic arm and be precisely controlled through a PID controller. Furthermore, the availability of spare parts in the local market was considered essential to guarantee easy and cost-effective maintenance. Tests were conducted on an actual robotic arm, and the designed gripper was able to effectively grasp objects such as a soda can and a pencil. The results demonstrated that the adaptive gripper successfully achieved various types of grasping, offering a scalable and economical solution that represents a significant contribution to the field of robotic manipulation in industrial applications. Full article
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<p>Open-source 3D Printed Three-Fingered Robotic Gripper.</p>
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<p>Diagram of the 3-finger robotic gripper kinematic structure. The central finger (S1) operates with two revolute joints (1A and 1B), allowing it to move similarly to a 2-joint planar articulated robot. The outer fingers (S2 and S3) also feature two revolute joints each (2A, 2B and 3A, 3B), along with additional joints (C+ and C−) that allow rotation around their base.</p>
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<p>Diagram of the Three-Fingered Gripper design. Half-cut view of the gripper (<b>a</b>), showing its main components: the finger rotational mechanism (<b>b</b>), where direct current (DC) micro motors control the rotation of the thumb and intermediate links (0° to 135°) using a gear mechanism and Hall effect sensors for precise movement; the bevel gear system (<b>c</b>), which enables the outer fingers to rotate around their own axes (0° to 90°); and the flexible membranes (<b>d</b>), which distribute pressure to the force sensors (FSR 402, FSR 406) through linear spaces that allow material bending.</p>
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<p>Stress analysis performed on one of the fingers of the gripper using Autodesk Inventor: (<b>a</b>) Von Mises stress analysis of a fingertip under maximum motor torque. (<b>b</b>) Deformation analysis of the fingertip’s TPU membrane. The design and patterns of the TPU membrane of the fingers must be able to perform a smooth and precise grip on objects.</p>
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<p>Force diagram at a point of contact, showing a top view, an isometric view, and the free body diagram (FBD) of the contact point. The forces F1, F2, and F3 act tangentially with the object and the friction between the finger membrane and the object surface, producing a stable and precise grip.</p>
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<p>Diagram of the gripper system hardware, showing controllers, sensors, and actuators.</p>
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<p>Gripper closed-loop control system block diagram.</p>
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<p>Grip positions: (<b>a</b>) open in three basic grip configurations (flat, cylindrical-spherical and tangential-flat), (<b>b</b>) closed gripper in base configurations, and (<b>c</b>) maximum working volume for each contact grip configuration at the base of the palm.</p>
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<p>Simulation in Autodesk Inventor showing the gripper transporting various objects (a soda can, Rubik’s cube, box, and pencil) between different positions over a table.</p>
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<p>Real environment pictures of a gripper mounted on an ABB IRB2600 industrial robot, displaying three gripping configurations: flat, cylindrical-spherical, and pincer. In the last row the gripper is also holding a soda can and a pencil for a verification test Screenshots from a video showing the ABB IRB2600 industrial robot using the gripper. The images illustrate the gripper performing three gripping actions: picking up a soda can, a pencil, and a rectangular object, corresponding to the cylindrical, pincer, and flat grips, respectively.</p>
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10 pages, 2775 KiB  
Proceeding Paper
Advancement of Electrospun Carbon Nanofiber Mats in Sensor Technology for Air Pollutant Detection
by Al Mamun, Mohamed Kiari, Abdelghani Benyoucef and Lilia Sabantina
Eng. Proc. 2024, 67(1), 82; https://doi.org/10.3390/engproc2024067082 - 3 Jan 2025
Viewed by 280
Abstract
The use of electrospun carbon nanofibers (ECNs) has been the focus of considerable interest due to their potential implementation in sensing. These ECNs have unique structural and morphological features such as high surface area-to-volume ratio, cross-linked pore structure, and good conductivity, making them [...] Read more.
The use of electrospun carbon nanofibers (ECNs) has been the focus of considerable interest due to their potential implementation in sensing. These ECNs have unique structural and morphological features such as high surface area-to-volume ratio, cross-linked pore structure, and good conductivity, making them well suited for sensing applications. Electrospinning technology, in which polymer solutions or melts are electrostatically deposited, enables the production of high-performance nanofibers with tailored properties, including fiber diameter, porosity, and composition. This controllability enables the use of ECNs to optimize sensing applications, resulting in improved sensor performance and sensitivity. While carbon nanofiber mats have potential for sensor applications, several challenges remain to improve selectivity, sensitivity, stability and scalability. Sensor technologies play a critical role in the global sharing of environmental data, facilitating collaboration to address transboundary pollution issues and fostering international cooperation to find solutions to common environmental challenges. The use of carbon nanofibers for the detection of air pollutants offers a variety of possibilities for industrial applications in different sectors, ranging from healthcare to materials science. For example, optical, piezoelectric and resistive ECNs sensors effectively monitor particulate matter, while chemoresistive and catalytic ECNs sensors are particularly good at detecting gaseous pollutants. For heavy metals, electrochemical ECNF sensors offer accurate and reliable detection. This brief review provides in-sights into the latest developments and findings in the fabrication, properties and applications of ECNs in the field of sensing. The efficient utilization of these resources holds significant potential for meeting the evolving needs of sensing technologies in various fields, with a particular focus on air pollutant detection. Full article
(This article belongs to the Proceedings of The 3rd International Electronic Conference on Processes)
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<p>(<b>a</b>) Atomic force microscopy (AFM) image of magnetic electrospun nanofiber mat. The scale bar shows 5 μm; (<b>b</b>) confocal laser scanning microscope (CLSM) image showing the PAN/gelatin nanofiber mats on a 3D-printed sample. The scale indicates 50 μm.</p>
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<p>Schematic of experimental setup for the fabrication of ZnO-MWCNT nanocomposite sensor and its ammonia gas sensing properties at room temperature. Reprinted from [<a href="#B56-engproc-67-00082" class="html-bibr">56</a>], with permission from Elsevier.</p>
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16 pages, 2495 KiB  
Article
A Novel Architecture for Addressing the Throughput Bottleneck in Spaceborne Solid-State Recorder for Electromagnetic Spectrum Sensors
by Xufeng Li, Li Zhou and Yan Zhu
Remote Sens. 2025, 17(1), 138; https://doi.org/10.3390/rs17010138 - 3 Jan 2025
Viewed by 204
Abstract
The data acquisition rate of electromagnetic spectrum sensors is exceedingly high. However, the throughput of current high-speed spaceborne solid-state recorders (S-SSR) remains relatively low, making it difficult for the data to be fully stored. To address this issue, a novel architecture for a [...] Read more.
The data acquisition rate of electromagnetic spectrum sensors is exceedingly high. However, the throughput of current high-speed spaceborne solid-state recorders (S-SSR) remains relatively low, making it difficult for the data to be fully stored. To address this issue, a novel architecture for a high-speed S-SSR is introduced in this study. The throughput of the S-SSR is primarily limited by three factors: the performance of the error-checking algorithm, the inability of a single FPGA to support the parallel expansion of too many Flash chips due to its limited effective I/O pins, and the efficiency of FLASH control. In the proposed architecture, a 10-stage pipelined RS(252,256) code is implemented. Data are distributed and stored in different memory regions controlled by separate FPGAs. Interleaved storage, multi-plane, and cache operation FLASH control module are also employed to resolve these bottlenecks. To further increase the throughput of the S-SSR, the system clock distribution has been optimized. In addition, interleaved encoding technology has been applied to improve radiation resistance and ensure data integrity. The performance of the system was evaluated on the Xilinx XC7K325T platform. The results confirm that the architecture is capable of handling high data rates and effectively correcting errors. The system can achieve a throughput of 46.8948 Gbps, making it suitable for future deployment in space exploration missions. Full article
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<p>System architecture of the high-speed S-SSR. This diagram presents the integrated setup of the S-SSR, showcasing the distribution of data management across multiple FPGAs.</p>
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<p>Implementation of the RS(256,252) algorithm in a cyclic XOR architecture. This operational flowchart illustrates the detailed computational process of the algorithm from start to end.</p>
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<p>Detailed view of the 10-stage pipeline structure of the RS(256252) algorithm. This figure illustrates the implementation of the algorithm from <a href="#remotesensing-17-00138-f002" class="html-fig">Figure 2</a> in a pipelined architecture. The relevant code for this module has been open-sourced from Github (<a href="https://github.com/lixuf/ECC_array/tree/main" target="_blank">https://github.com/lixuf/ECC_array/tree/main</a> (accessed on 1 January 2024)).</p>
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<p>Timing diagram illustrating the processing and output of RS(256252) error control module.</p>
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<p>Implementation of interleaving unit. This figure demonstrates how the four interleaving methods are output in a pipelined manner using multiplexers.</p>
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<p>Example of resilience against bit-upset. This figure provides an example of how various bit-upset events are distributed across multiple error-correction sequences.</p>
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<p>Detailed view of the storage area implementation: In the figure, the data lines are shared between two groups of chips, while the control lines are used independently by each group.</p>
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<p>Illustration showing the data programming process between two groups of FLASH chips with concealed overhead.</p>
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<p>Patterns of bit upset events, including double-bit, triple-bit, quadruple-bit, and quintuple-bit upsets. (<b>a</b>–<b>c</b>) Patterns of double-bit upsets. (<b>d</b>–<b>f</b>) Patterns of triple-bit upsets. (<b>g</b>–<b>k</b>) Patterns of quadruple-bit upsets. (<b>l</b>) Pattern of quintuple-bit upsets.</p>
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10 pages, 4642 KiB  
Article
Preparation and Applications of Multifunctional MXene/Tussah Silk Fabric
by Bingbing Xu, Yue Zhang, Jia Li, Boxiang Wang, Yanhua Lu and Dehong Cheng
Materials 2025, 18(1), 169; https://doi.org/10.3390/ma18010169 - 3 Jan 2025
Viewed by 288
Abstract
The development of functional textiles has become a key focus in recent years, aiming to meet the diverse requirements of modern society. MXene has excellent conductivity, hydrophilicity, and UV resistance, and is widely used in electromagnetic shielding, sensors, energy storage, and photothermal conversion. [...] Read more.
The development of functional textiles has become a key focus in recent years, aiming to meet the diverse requirements of modern society. MXene has excellent conductivity, hydrophilicity, and UV resistance, and is widely used in electromagnetic shielding, sensors, energy storage, and photothermal conversion. Tussah silk (TS) is a unique natural textile raw material and has a unique jewelry luster, natural luxury, and a smooth and comfortable feel. However, there are relatively few studies on the functional finishing of TS fabric with Ti3C2Tx MXene. Here, we developed a multifunctional MXene/tussah silk (MXene/TS) fabric by the deposition of Ti3C2Tx MXene sheets on the surface of TS fabric through a simple padding–drying–curing process. The obtained MXene/TS fabric (five cycles) exhibited excellent conductivity (4.8 S/m), air permeability (313.6 mm/s), ultraviolet resistance (ultraviolet protection factor, UPF = 186.3), photothermal conversion (temperature increase of 11 °C), and strain sensing. Thanks to these superior properties, the MXene/TS fabric has broad application prospects in motion monitoring, smart clothing, flexible wearables, and artificial intelligence. Full article
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<p>Schematic illustration of the fabrication process of the MXene/TS fabric.</p>
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<p>SEM image of (<b>a</b>) Ti<sub>3</sub>AlC<sub>2</sub>, (<b>b</b>) multilayer Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub>, and (<b>c</b>) delaminated Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> nanosheets. (<b>d</b>) Dynamic light scattering (DLS) size distribution of Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> nanosheets.</p>
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<p>SEM images of (<b>a</b>–<b>c</b>) TS fabric and (<b>d</b>–<b>f</b>) MXene/TS fabric at different resolutions.</p>
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<p>Conductivity of MXene/TS fabric at different (<b>a</b>) impregnation time, (<b>b</b>) curing time, (<b>c</b>) curing temperature, (<b>d</b>) cycles of two-dipping and two-rolling with PDDA, (<b>e</b>) cycles of two-dipping and two-rolling without PDDA. (<b>f</b>) Loading of MXene under different impregnation cycles.</p>
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<p>(<b>a</b>) Reflectance, (<b>b</b>) K/S value, (<b>c</b>) air permeability, (<b>d</b>) UV transmittance, and (<b>e</b>) UPF of fabric with different finishing times. (<b>f</b>) UV–Vis spectrum of Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> MXene.</p>
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<p>(<b>a</b>) Schematic diagram of photothermal conversion of MXene/TS fabric. (<b>b</b>) Photothermal conversion properties of TS and MXene/TS fabric. (<b>c</b>) Applications of the MXene/TS fabric strain sensor for various physiological signal detection. Relative resistance curves during (<b>d</b>) finger bending, (<b>e</b>) wrist bending, and (<b>f</b>) knee bending.</p>
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17 pages, 5024 KiB  
Article
Comparative Study of γ Radiation-Induced Effects on Fiber Bragg Gratings by Femtosecond Laser Point-by-Point Method and Line-by-Line Method
by Mingyang Hou, Yumin Zhang, Xin Xiong and Lianqing Zhu
Photonics 2025, 12(1), 32; https://doi.org/10.3390/photonics12010032 - 3 Jan 2025
Viewed by 305
Abstract
In the realm of advanced optical fiber sensing (OFS) technologies, Fiber Bragg Grating (FBG) has garnered widespread application in the monitoring of temperature, strain, and external refractive indices, particularly within high-radiation environments such as high-energy physics laboratories, nuclear facilities, and space satellites. Notably, [...] Read more.
In the realm of advanced optical fiber sensing (OFS) technologies, Fiber Bragg Grating (FBG) has garnered widespread application in the monitoring of temperature, strain, and external refractive indices, particularly within high-radiation environments such as high-energy physics laboratories, nuclear facilities, and space satellites. Notably, FBGs inscribed using femtosecond lasers are favored for their superior radiation resistance. Among various inscription techniques, the point-by-point (PbP) and line-by-line (LbL) methods are predominant; however, their comparative impacts on radiation durability have not been adequately explored. In this research, FBGs were inscribed on a single-mode fiber using both the PbP and LbL methods, and subsequently subjected to a total irradiation dose of 5.04 kGy (radiation flux of 2 rad/s) over 70 h in a 60Co-γ radiation environment. By evaluating the changes in temperature- and strain-sensing performance of the FBG pre-irradiation and post-irradiation, this study identifies a more favorable technique for writing anti-irradiation FBG sensors. Moreover, an analysis into the radiation damage mechanisms in optical fibers, alongside the principles of femtosecond laser inscription, provides insights into the enhanced radiation resistance observed in femtosecond laser-written FBGs. This study thus furnishes significant guidance for the development of highly radiation-resistant FBG sensors, serving as a critical reference in the field of high-performance optical fiber sensing technologies. Full article
(This article belongs to the Special Issue Emerging Trends in Optical Fiber Sensors and Sensing Techniques)
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<p>Schematic diagram of FBG sensing principle.</p>
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<p>Schematic of femtosecond inscription FBG.</p>
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<p>Micrograph of writing FBG by femtosecond laser.</p>
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<p>Schematic of sensing experiment.</p>
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<p>Sensing experiment setup.</p>
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<p>Schematic of radiation experiment.</p>
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<p>Temperature-sensing spectral diagram and central wavelength drift diagram written by the PbP method before irradiation: (<b>a</b>) 3d spectrum of heating; (<b>b</b>) center wavelength drift diagram of heating; (<b>c</b>) 3d spectrum of cooling; (<b>d</b>) center wavelength drift diagram of cooling.</p>
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<p>Temperature-sensing spectral diagram and central wavelength drift diagram written by the PbP method after irradiation: (<b>a</b>) 3d spectrum of heating; (<b>b</b>) center wavelength drift diagram of heating; (<b>c</b>) 3d spectrum of cooling; (<b>d</b>) center wavelength drift diagram of cooling.</p>
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<p>The strain-sensing spectrum and the central wavelength drift diagram written by the PbP method before irradiation: (<b>a</b>) 3d spectrum of applying strain; (<b>b</b>) center wavelength drift diagram of applying strain; (<b>c</b>) 3d spectrum of unloading strain; (<b>d</b>) center wavelength drift diagram of unloading strain.</p>
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<p>The strain-sensing spectrum and the central wavelength drift diagram written by the PbP method after irradiation: (<b>a</b>) 3d spectrum of applying strain; (<b>b</b>) center wavelength drift diagram of applying strain; (<b>c</b>) 3d spectrum of unloading strain; (<b>d</b>) center wavelength drift diagram of unloading strain.</p>
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13 pages, 3375 KiB  
Article
Effect of Deposition Temperature and Thermal Annealing on the Properties of Sputtered NiOx/Si Heterojunction Photodiodes
by Roumen Nedev, David Mateos-Anzaldo, Eddue Osuna-Escalante, Oscar Perez-Landeros, Mario Curiel-Alvarez, Esteban Osorio-Urquizo, Jhonathan Castillo-Saenz, Javier Lopez-Medina, Benjamin Valdez-Salas and Nicola Nedev
Inorganics 2025, 13(1), 11; https://doi.org/10.3390/inorganics13010011 - 3 Jan 2025
Viewed by 249
Abstract
NiOx is a p-type semiconductor with excellent stability, which makes it interesting for a wide range of applications. Broadband photodetectors with high responsivity (R) were fabricated by depositing r.f.-sputtered NiOx layers on n-Si at room temperature (RT), 50 °C [...] Read more.
NiOx is a p-type semiconductor with excellent stability, which makes it interesting for a wide range of applications. Broadband photodetectors with high responsivity (R) were fabricated by depositing r.f.-sputtered NiOx layers on n-Si at room temperature (RT), 50 °C and 100 °C. In self-powered mode the RT diodes have R between 0.95 and 0.39 A/W for wavelengths between 365 and 635 nm, while at a reverse bias of −4 V, the responsivity increases to values between 22 A/W and 10.7 A/W for wavelengths in the same range. The increase of the deposition temperature leads to a decrease of R but also to a smaller reverse dark current. Thus, the 100 °C photodiodes might be more appropriate for applications where high responsivity is required, because of their smaller power consumption compared to the RT diodes. In addition, it was found that the increase of the deposition temperature leads to an increase of the diodes’ series resistance and the resistivity of NiOx. The effect of Rapid Thermal Annealing (RTA) on the properties of the photodiodes was studied. Annealing at 550 °C for 6 min leads to much higher responsivity compared to R of diodes with as-deposited NiOx. However, a disadvantage of the annealed diode is that the reverse current depends on the amplitude and polarity of previously applied bias voltage. The higher responsivity of the RTA photodiodes makes them useful as light sensors. Full article
(This article belongs to the Special Issue Advanced Inorganic Semiconductor Materials, 2nd Edition)
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<p>(<b>a</b>) Experimental Ψ and Δ dependences and the fitted curves for a layer deposited at 100 °C and subjected to RTA. Refractive index for: (<b>b</b>) As-deposited layers; (<b>c</b>) RTA annealed layers.</p>
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<p>(<b>a</b>) Transmittance of CG substrate and CG coated with NiO<span class="html-italic"><sub>x</sub></span> layers deposited at RT, 50 °C and 100 °C; (<b>b</b>) band gaps of the films determined by the Tauc plot method.</p>
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<p>AFM results of as-deposited NiO<span class="html-italic"><sub>x</sub></span> layers obtained at: (<b>a</b>) RT, (<b>b</b>) 50 °C and (<b>c</b>) 100 °C and of RTA annealed layers deposited at: (<b>d</b>) RT, (<b>e</b>) 50 °C and (<b>f</b>) 100 °C.</p>
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<p>Schematic diagram of the structure of the studied devices with definition of the bias voltage polarity.</p>
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<p><span class="html-italic">I-V</span> characteristics of photodiodes with NiO<span class="html-italic"><sub>x</sub></span> layers deposited at: (<b>a</b>) RT, (<b>b</b>) 50 °C and (<b>c</b>) 100 °C measured in the dark and under illumination with red, green, blue and UV light.</p>
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<p>Schematic energy band diagram of a p-NiO<span class="html-italic"><sub>x</sub></span>/n-Si diode under short-circuit conditions, <span class="html-italic">V</span> = 0 V.</p>
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<p><span class="html-italic">I-V</span> characteristics of photodiodes with NiO<span class="html-italic"><sub>x</sub></span> layers deposited at: (<b>a</b>) RT, (<b>b</b>) 50 °C and (<b>c</b>) 100 °C and subjected to RTA annealing. The dependences were measured in the dark and under illumination with red, green, blue and UV light. The inset in (<b>b</b>) shows a zoomed view of the current in the region of −0.5–0.5 V of a characteristic measured between 5 V and −10 V and then in the opposite direction.</p>
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<p><span class="html-italic">C-V</span> characteristics measured in the dark under reverse bias of: (<b>a</b>) diodes with as-deposited NiO<span class="html-italic"><sub>x</sub></span> layers; (<b>b</b>) diodes with RTA annealed layers.</p>
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<p>Time-dependent photoresponses of diodes with as-deposited NiO<span class="html-italic"><sub>x</sub></span> layers obtained at: (<b>a</b>) RT, (<b>b</b>) 50 °C, and (<b>c</b>) 100 °C, and of diodes with RTA annealed layers deposited at: (<b>d</b>) RT, (<b>e</b>) 50 °C, and (<b>f</b>) 100 °C. The switching curves of the diodes with as-deposited layers were measured at voltage pulses of −3 V, while the RTA diodes were measured at pulses of <span class="html-italic">V<sub>r</sub></span> = −8 V. The red, green, blue and violet color lines correspond to illumination with red, green, blue and UV LED, respectively.</p>
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<p>(<b>a</b>) <span class="html-italic">I</span>/<span class="html-italic">g</span> vs. <span class="html-italic">I</span> dependencies for diodes with as-deposited NiO<span class="html-italic"><sub>x</sub></span> layers prepared at RT, 50 °C and 100 °C. Higher line slope corresponds to higher <span class="html-italic">R<sub>s</sub></span>; (<b>b</b>) comparison of the <span class="html-italic">I</span>/<span class="html-italic">g</span> vs. <span class="html-italic">I</span> dependences for a diode with as-deposited NiO<span class="html-italic"><sub>x</sub></span> prepared at 100 °C (red line) and a RTA annealed diode with NiO<span class="html-italic"><sub>x</sub></span> layer deposited at RT (black line). Note the difference in <span class="html-italic">x</span>-axis scale.</p>
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<p>Responsivity of photodiodes with: (<b>a</b>) as-deposited NiO<span class="html-italic"><sub>x</sub></span> layers; (<b>b</b>) RTA annealed NiO<span class="html-italic"><sub>x</sub></span> layers.</p>
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31 pages, 7617 KiB  
Review
Polymer Composites with Nanomaterials for Strain Gauging: A Review
by Aleksei V. Shchegolkov, Alexandr V. Shchegolkov, Vladimir V. Kaminskii and Maxim A. Chumak
J. Compos. Sci. 2025, 9(1), 8; https://doi.org/10.3390/jcs9010008 - 2 Jan 2025
Viewed by 624
Abstract
Strain gauges and strain gauge transducers are important tools in the field of material resistance research to measure the stresses and strains in solids. These methods and devices have a wide range of applications, from construction to mechanical engineering, where the mechanical properties [...] Read more.
Strain gauges and strain gauge transducers are important tools in the field of material resistance research to measure the stresses and strains in solids. These methods and devices have a wide range of applications, from construction to mechanical engineering, where the mechanical properties of materials need to be monitored and optimized. The use of nanomaterials in strain gauges allows for more sensitive and compact sensors. Nanotechnology makes it possible to create strain gauges with improved mechanical and electrical properties. At the same time, nanomaterials have unique properties that make them ideal for use in strain gauges. This paper considers different types of composites based on polymer matrices with additives of dispersed nanomaterials, which are designed for strain gauge tasks. Thermoplastics and elastomers can be used as polymer matrices. Dispersed fillers can be based on MXene and nanomaterials such as carbon nanotubes, graphene, metals, etc. Despite the obvious advantages of strain gauges based on conducting polymers modified with dispersed structures, there are problems in creating effective strain gauges with the ability to operate under large deformations with an improved sensitivity and accuracy of measurements in a wide range. This article also provides brief information on the technical evolution of strain gauges, from wire and foil to polymer nanocomposites. A modern classification of strain gauges is provided. The disadvantages and advantages of existing strain gauges are shown. The review contains information on commercial strain gauges. The mechanisms of electrical conductivity formation in polymer composites for strain gauges are described in detail. The areas of application of polymer nanocomposite strain gauges are also specified in detail. The purpose of this review study is to determine the prospects for the use of various nanomaterials as additives in polymers to create strain gauges. The review is aimed at a wide range of readers. Full article
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<p>Strain gauge design: (<b>a</b>)—in longitudinal section: 1—coating; 2—grid; 3—substrate; and 4—external lead; (<b>b</b>)—top view; and (<b>c</b>)—wire in section (0.001-inch diameter).</p>
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<p>Linear strain gauge: (<b>a</b>)—working principle of foil strain gauge: 1—wire grid; 2—support; 3—contacts; and L—base and (<b>b</b>)—wire-on-paper strain gauge (sample of the 60 s).</p>
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<p>Different applications of foil gauge strain gauges: (<b>a</b>) and (<b>b</b>)—single and (<b>c</b>)—multi-point.</p>
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<p>Hot beverage filling machine.</p>
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<p>Installation and mounting of column load cell ZSFY-A/-SS: 1—foundation; 2—lower baseplate; 3—duster; 4—upper cup; 5—upper baseplate; 6—loading platform; 7—M8 screw; 8—load cell; 9—lower cup; and 10—eccentric.</p>
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<p>Algorithm for selecting strain gauges for different applications.</p>
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<p>Types of strain gauge: (<b>a</b>)—foil; (<b>b</b>)—wire; and (<b>c</b>)—film (commercial device).</p>
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<p>Semiconductor strain gauge.</p>
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<p>Strain output of a high-temperature Pt thin-film thermistor at 700 °C, 5 cycles [<a href="#B69-jcs-09-00008" class="html-bibr">69</a>].</p>
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<p>Full-bridge circuit (simplified circuit).</p>
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<p>Load cells by the shape of the load-bearing base: (<b>a</b>)—cantilever; (<b>b</b>)—cylindrical; and (<b>c</b>)—S-shaped.</p>
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<p>Classification of strain gauges.</p>
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<p>Carbon nanostructures in different dimensions.</p>
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<p>Schematics of the MWCNT/PVA-based humidity sensor production process.</p>
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<p>Schematic for the alignment of CNTs in the composites by uniaxial stretching and network rearrangement.</p>
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<p>(<b>a</b>) Schematical illustration of a strain sensor based on CPHs and (<b>b</b>) the piezoresistivity mechanism of a PVA-PPy strain sensor when applying small strain.</p>
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<p>Percolation process in conductive composites.</p>
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<p>Structure of the conductive polymer nanocomposite before and after treatment: (<b>a</b>)—before treatment of CNTs in the polymer, pronounced agglomeration of CNT particles; and (<b>b</b>)—treated CNTs in the polymer, conductive phase.</p>
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<p>Schematic diagram of the dependence of logarithmic conductivity on the concentration of CNTs (vol. %), illustrating the S-shaped percolation curve.</p>
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17 pages, 11338 KiB  
Article
Fabrication and Electrical Characterization of Low-Temperature Polysilicon Films for Sensor Applications
by Filipa C. Mota, Inês S. Garcia, Aritz Retolaza, Dimitri E. Santos, Patrícia C. Sousa, Diogo E. Aguiam, Rosana A. Dias, Carlos Calaza, Alexandre F. Silva and Filipe S. Alves
Micromachines 2025, 16(1), 57; https://doi.org/10.3390/mi16010057 - 31 Dec 2024
Viewed by 384
Abstract
The development of low-temperature piezoresistive materials provides compatibility with standard silicon-based MEMS fabrication processes. Additionally, it enables the use of such material in flexible substrates, thereby expanding the potential for various device applications. This work demonstrates, for the first time, the fabrication of [...] Read more.
The development of low-temperature piezoresistive materials provides compatibility with standard silicon-based MEMS fabrication processes. Additionally, it enables the use of such material in flexible substrates, thereby expanding the potential for various device applications. This work demonstrates, for the first time, the fabrication of a 200 nm polycrystalline silicon thin film through a metal-induced crystallization process mediated by an AlSiCu alloy at temperatures as low as 450 °C on top of silicon and polyimide (PI) substrates. The resulting polycrystalline film structure exhibits crystallites with a size of approximately 58 nm, forming polysilicon (poly-Si) grains with diameters between 1–3 µm for Si substrates and 3–7 µm for flexible PI substrates. The mechanical and electrical properties of the poly-Si were experimentally conducted using microfabricated test structures containing piezoresistors formed by poly-Si with different dimensions. The poly-Si material reveals a longitudinal gauge factor (GF) of 12.31 and a transversal GF of −4.90, evaluated using a four-point bending setup. Additionally, the material has a linear temperature coefficient of resistance (TCR) of −2471 ppm/°C. These results illustrate the potential of using this low-temperature film for pressure, force, or temperature sensors. The developed film also demonstrated sensitivity to light, indicating that the developed material can also be explored in photo-sensitive applications. Full article
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<p>Illustration of the MIC process for non-silicide forming systems, which starts with (<b>a</b>) the diffusion of the Si atoms into the metal layer, followed by (<b>b</b>) the nucleation of the atoms into a crystalline structure, and finishing with (<b>c</b>) the achievement of a continuous poly-Si layer.</p>
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<p>SEM pictures of the poly-Si film obtained by annealing the AlSiCu(200 nm)/a-Si(250 nm) at 450 °C for 8 h (<b>a</b>) on top of a Si wafer and (<b>b</b>) on top of PI 4110-HD layer.</p>
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<p>SEM picture of the poly-Si obtained by annealing the AlSiCu (200 nm)/a-Si (250 nm) at 450 °C for 12 h on top of a PI layer.</p>
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<p>XRD measurements of the poly-Si film obtained showing a crystalline peak in the direction &lt;111&gt; at 2θ = 28.43° (<b>a</b>) directly on top of a Si wafer and (<b>b</b>) on top of PI HD-4410.</p>
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<p>BSE images of the poly-Si film obtained by annealing the AlSiCu (200 nm)/a-Si (250 nm) at 450 °C for 8 h (<b>a</b>) on top of a Si-wafer and (<b>b</b>) on top of PI 4110-HD layer.</p>
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<p>(<b>a</b>) Test structure containing three piezoresistors and the conductive paths for external measurements. (<b>b</b>) Illustration of the disposition of the three piezoresistors in each device: the top piezoresistor has a rotation of 0°, middle piezoresistor has a rotation of 90° and the bottom piezoresistor has a rotation of 135°.</p>
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<p>Flow-chart illustration of the fabrication process of the device containing poly-Si piezoresistors for electrical and mechanical characterization of the developed material: (<b>i</b>) developed poly-Si; (<b>ii</b>) patterning of the poly-Si film; (<b>iii</b>) AlSiCu sputtering; (<b>iv</b>) AlSiCu patterning and (<b>v</b>) deposition and patterning of SiO<sub>2</sub> passivation layer.</p>
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<p>I–V characteristic of the poly-Si piezoresistors with dimensions (<b>a</b>) L/W = 5, (<b>b</b>) L/W = 10 and (<b>c</b>) L/W = 20 extracted under dark and light environments.</p>
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<p>Electrical resistance stability measured for 6 h in a climate chamber at a temperature of 25 °C and humidity of 50% with input voltage signal of 5 V and 10 V for piezoresistors with L/W = 5, 10 and 20 normalized with the nominal resistance at 5 V for each piezoresistor.</p>
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<p>Resistance variation with temperature for piezoresistors with L/W = 5, 10 and 20.</p>
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<p>Illustration of a four-point bending set-up for the piezoresistive behavior characterization.</p>
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<p>Machined pieces for the (<b>a</b>) load beams and (<b>b</b>) support beams. (<b>c</b>) Positioning of the device in the set up.</p>
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<p>(<b>a</b>) Resistance change with strain of the piezoresistors oriented at 0° to extract the longitudinal GF. (<b>b</b>) Resistance change with strain of the piezoresistors oriented at 90° to extract the transversal GF.</p>
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23 pages, 2053 KiB  
Review
Research Progress in Fiber Bragg Grating-Based Ocean Temperature and Depth Sensors
by Xinyu Zhao, Chenxi Wei, Lina Zeng, Li Sun, Zaijin Li, Hao Chen, Guojun Liu, Zhongliang Qiao, Yi Qu, Dongxin Xu, Lianhe Li and Lin Li
Sensors 2025, 25(1), 183; https://doi.org/10.3390/s25010183 - 31 Dec 2024
Viewed by 322
Abstract
Fiber Bragg gratings (FBGs) are widely used in stress and temperature sensing due to their small size, light weight, high resistance to high temperatures, corrosion, electromagnetic interference, and low cost. In recent years, various structural enhancements and sensitization to FBGs have been explored [...] Read more.
Fiber Bragg gratings (FBGs) are widely used in stress and temperature sensing due to their small size, light weight, high resistance to high temperatures, corrosion, electromagnetic interference, and low cost. In recent years, various structural enhancements and sensitization to FBGs have been explored to improve the performance of ocean temperature and depth sensors, thereby enhancing the accuracy and detection range of ocean temperature and depth data. This paper reviews advancements in temperature, pressure, and dual-parameter enhancement techniques for FBG-based sensors. Additionally, the advantages and disadvantages of each method are compared and analyzed, providing new directions for the application of FBG sensors in marine exploration. Full article
(This article belongs to the Section Optical Sensors)
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<p>Principle of Fiber Bragg Grating Reflection and Transmission [<a href="#B38-sensors-25-00183" class="html-bibr">38</a>].</p>
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<p>Spectral Shift in Fiber Bragg Grating under External Influences [<a href="#B40-sensors-25-00183" class="html-bibr">40</a>].</p>
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<p>Schematic Diagram of Pressure Sensor Structure [<a href="#B74-sensors-25-00183" class="html-bibr">74</a>].</p>
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<p>(<b>a</b>–<b>c</b>) Principle and Physical Diagram of π-FBG Sensor [<a href="#B67-sensors-25-00183" class="html-bibr">67</a>].</p>
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<p>Schematic Diagram of the Structure of an FBG Pressure Sensor [<a href="#B84-sensors-25-00183" class="html-bibr">84</a>].</p>
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<p>Schematic Diagram of the Sensor Structure Based on Membrane and Lever [<a href="#B86-sensors-25-00183" class="html-bibr">86</a>].</p>
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27 pages, 11281 KiB  
Article
Pre-Occupancy Evaluation of Affective Experiences in Building Information Modeling Through SLR and an e-Delphi Survey
by Balamaheshwaran Renganathan, Radhakrishnan Shanthi Priya and Ramalingam Senthil
Technologies 2025, 13(1), 14; https://doi.org/10.3390/technologies13010014 - 30 Dec 2024
Viewed by 427
Abstract
Building information modeling (BIM) is increasingly used during the conceptual design phase, which focuses on simulations such as energy usage analysis and comfort levels, like temperature and lighting conditions, to enhance user experience and well-being, which are key factors for meeting Sustainable Development [...] Read more.
Building information modeling (BIM) is increasingly used during the conceptual design phase, which focuses on simulations such as energy usage analysis and comfort levels, like temperature and lighting conditions, to enhance user experience and well-being, which are key factors for meeting Sustainable Development Goal 3. This study employs a systematic literature review and an e-Delphi survey to explore how a pre-occupancy evaluation integrated within BIM frameworks addresses affective responses and suggests ways to improve design decisions that align with the UN’s sustainable development goals. The study identified a research gap in how BIM evaluations are conducted during the conceptual design stage, including crucial sensory aspects for human well-being. The research suggests incorporating evidence-based design instruments like body sensor networks (BSN) and immersive virtual reality and methods like neurophenomenology to enhance the assessment of user interactions in the design process. Prioritizing the human-centered design approach right from the start can facilitate the integration of innovative workflows into architecture, engineering, and construction practices. Overcoming resistance to these workflows and methodologies is essential for advancing BIM’s role in fostering spatial environments that support health, well-being, and positive affective experiences. Full article
(This article belongs to the Section Construction Technologies)
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<p>Structure of the present work.</p>
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<p>Outlines of the research design used in this study.</p>
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<p>PRISMA flow chart of the SLR.</p>
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<p>Network visualization of keyword co-occurrence analysis, map generated in VOS viewer.</p>
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<p>Overview of the results from the e-Delphi process (Round 1–3).</p>
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<p>Representation of key statistical data of e-Delphi survey rounds 2 (R2).</p>
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<p>Representation of key statistical data of e-Delphi survey rounds 3 (R3).</p>
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<p>Findings from the SLR and e-Delphi survey.</p>
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<p>Locating the identified knowledge gap through SLR and e-Delphi survey.</p>
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21 pages, 5252 KiB  
Article
A Multi-Layered Origami Tactile Sensory Ring for Wearable Biomechanical Monitoring
by Rajat Subhra Karmakar, Hsin-Fu Lin, Jhih-Fong Huang, Jui-I Chao, Ying-Chih Liao and Yen-Wen Lu
Biosensors 2025, 15(1), 8; https://doi.org/10.3390/bios15010008 - 27 Dec 2024
Viewed by 599
Abstract
An origami-based tactile sensory ring utilizing multilayered conductive paper substrates presents an innovative approach to wearable health applications. By harnessing paper’s flexibility and employing origami folding, the sensors integrate structural stability and self-packaging without added encapsulation layers. Knot-shaped designs create loop-based systems that [...] Read more.
An origami-based tactile sensory ring utilizing multilayered conductive paper substrates presents an innovative approach to wearable health applications. By harnessing paper’s flexibility and employing origami folding, the sensors integrate structural stability and self-packaging without added encapsulation layers. Knot-shaped designs create loop-based systems that secure conductive paper strips and protect sensing layers. Demonstrating a sensitivity of 3.8 kPa−1 at subtle pressures (0–0.05 kPa), the sensors detect both minimal stimuli and high-pressure inputs. Electrical modeling of various origami configurations identifies designs with optimized performance with a pentagon knot offering higher sensitivity to support high-sensitivity needs. Meanwhile a square knot provides greater precision and quicker recovery, balancing sensitivity and stability for real-time feedback devices. The enhanced elastic modulus from folds remains within human skin’s elasticity range, ensuring comfort. Applications include grip strength monitoring and pulse rate detection from the thumb, capturing pulse transit time (PTT), an essential cardiovascular biomarker. This design shows the potential of origami-based tactile sensors in creating versatile, cost-effective wearable health monitoring systems. Full article
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<p>Origami tactile sensors with three different structures and their conduction mechanism: (<b>a</b>) Preparation of conductive paper by Screen printing process. (<b>b</b>) Schematic diagram of Love-knot, Square-knot, and Pentagon-knot origami structure. Airlaid paper was used as substrate with the graphene ink used as sensing material. (<b>c</b>) ECR variation mechanism for tactile sensing.</p>
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<p>Material properties data: (<b>a</b>) SEM image of uncoated airlaid paper. (<b>b</b>) SEM image of screen-printed airlaid paper. (<b>c</b>) The magnified view of a single fiber, which shows the infusion of conductive ink into the fibrous structure of the substrate. (<b>d</b>) C1s and (<b>e</b>) O1s peaks of XPS spectra of conductive composite films. The deconvolution of these peaks were done to understand the bonds present in the material. (<b>f</b>) Raman spectra of conductive composite films showing the material composition of both inks. The D, G and 2D bands were explored to understand the presence of graphene layers.</p>
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<p>Circuit representation of Origami Tactile sensor. (<b>a</b>) The front and back side schematic of Love-knot origami tactile sensor (S1) showing the symmetrical arrangement of sensing layers. The real-time image of sensing device is also presented here. (<b>b</b>) The circuit representation of Love-knot structure. (<b>c</b>) The schematic diagram of Square-knot origami tactile sensor along with the real-time photograph of the device. (<b>d</b>) The circuit representation of Square-knot structure for three different configurations based on interfacial resistive layers’ numbers i.e., S2, S3 and S4. To identify those layers, the face-to-face arranged conductive papers were marked red borderline in this schematic. (<b>e</b>) The front and back side schematic of Pentagon-knot origami tactile sensor (S5), which also demonstrates the symmetrical arrangement of sensing layers. The real-time image of sensing device is also presented here. (<b>f</b>) The circuit representation of Pentagon-knot structure.</p>
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<p>Resistive sensing characteristics of Origami tactile sensors. (<b>a</b>) The comparison of recorded initial resistance (R<sub>0</sub>) value of all five origami sensor configuration along with the R<sub>0</sub> value of single sensing layer. Normalized resistance (R/R<sub>0</sub>) changes with applied pressure for all the origami tactile sensors for (<b>b</b>) the entire pressure range of 0–200 kPa and (<b>c</b>) low pressure region i.e., 0–5 kPa. (<b>d</b>) Sensitivity data of all five different fabricated sensors for three different pressures. (<b>e</b>) The co-efficient of variation data of all fabricated Origami tactile sensors indicating the stability and repeatability of sensor measurements. (<b>f</b>) The degree of hysteresis of all fabricated Origami tactile sensors indicating the accuracy of fabricated sensors. (<b>g</b>) Reversible testing for 2000 cycles of repeated loading and unloading of medium (10 kPa) and high (200 kPa) applied pressures. (<b>h</b>) Five number of cycles from medium- and high-pressure regions. (<b>i</b>) The relative ECR values of all fabricated origami sensors at 10 and 200 kPa to understand the resistance deviation in the end of loading-unloading cycle. The time-dependent resistance characteristics for tactile sensors with (<b>j</b>) 10 kPa and (<b>k</b>) 200 kPa applies pressure for one cycle. (<b>l</b>) The Recovery time of all five different sensors calculate from the time-dependent resistive data for one cycle.</p>
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<p>Comparison between origami structured tactile sensing device and planner sensing devices. (<b>a</b>) The resistive characteristics data of planner and origami tactile sensors for dual interfacial layers and quadruple interfacial layers. (<b>b</b>) The sensitivity comparison for 0.05 kPa and 1 kPa applied pressure. (<b>c</b>) The Formation method of Origami tactile sensing ring. It was created by using the extended paper strip to form a loop around the finger. Two sensors (S2 and S5) were selected as shown in the inset. The placement of origami ring was also demonstrated here. (<b>d</b>) Demonstration of wearable application by performing the grasping test by using two different objects, i.e., Tennis Ball and Rubber Bellow respectively.</p>
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<p>Grip Strength Monitoring. (<b>a</b>) Experimental set up of grip strength monitoring. (<b>b)</b> The close-up image of hand to show the origami ring location. (<b>c</b>) Isometric results of dynamometer and origami ring with S2 and S5 for three different applied force. (<b>d</b>) Isotonic test results of dynamometer and origami ring with S2 and S5 at rapid press and release movement. (<b>e</b>) Experimental set up of pulse rate monitoring. (<b>f</b>) The close-up image of hand to show the origami ring location. (<b>g</b>) Pulse-rate data detected by S2 and S5 origami ring compared to a standard ECG signal obtained simultaneously. (<b>h</b>) The three peaks of both pulse rate and ECG signal were emphasized for analyzing the pulse transit time (PTT).</p>
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22 pages, 6872 KiB  
Article
Improved Interconnected MRAS Parameter Identification for Speed Sensorless Control of Linear Induction Motor
by Hailin Hu, Shiyan Yu, Liangjie Ren, Mingda Zhai and Yuhui Chen
Actuators 2025, 14(1), 2; https://doi.org/10.3390/act14010002 - 26 Dec 2024
Viewed by 271
Abstract
After eliminating the speed sensor in the linear induction motor (LIM) high-performance closed-loop control system, the speed feedback information is missing in the speed closed loop. The accuracy of speed observation results is affected by changes in magnetizing inductance and primary resistance. This [...] Read more.
After eliminating the speed sensor in the linear induction motor (LIM) high-performance closed-loop control system, the speed feedback information is missing in the speed closed loop. The accuracy of speed observation results is affected by changes in magnetizing inductance and primary resistance. This effect can cause significant oscillations in the results of the speed sensorless control system, preventing them from converging. An enhanced model reference adaptive system (MRAS) multi-parameter parallel identification methodology based on the interconnected second-order super-twisting algorithm (SOSTA) is proposed. To enhance the system’s dynamic performance, we designed an improvement to the MRAS observer based on the SOSTA, with a focus on the LIM state-space equation that considers dynamic edge-end effects. The impact of parameter alterations on the LIM system is examined. To improve speed observation accuracy and system stability, a two-parameter MRAS identification model was created. The Popov hyperstability principle was used to formulate control laws for these two parameters, ultimately enabling the identification of these two parameters. The identified values were fed back to the speed observation and control system, which reduces the coupling of these two parameters and speed. Simulation and hardware-in-the-loop experiments demonstrate that the observation system estimates speed accurately when these two parameters undergo abrupt changes within the rated speed range, enhancing the precision and robustness of the speed sensorless control system. Full article
(This article belongs to the Special Issue Advanced Theory and Application of Magnetic Actuators—2nd Edition)
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Figure 1

Figure 1
<p>Space vector T-type equivalent circuit of LIM.</p>
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<p>Second-order super-twisting sliding mode observer model.</p>
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<p>Distribution of LIM root trajectories under variation in magnetizing inductance or primary resistance parameters: (<b>a</b>) The impact of varying the magnetizing inductance by a factor of 0.5 versus 1.5 on the poles. (<b>b</b>) The impact of varying the primary resistance by a factor of 0.5 versus 1.5 on the poles.</p>
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<p>Observer structure diagram based on improved interconnected MRAS.</p>
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<p>LIM interconnected MRAS observer system block diagram.</p>
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<p>Flowchart of realization of discrete second-order super-twisting sliding mode observer.</p>
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<p>Improved MRAS speed estimation accelerates to 10 m/s simulation results. (<b>a</b>) Speed response plot for <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi mathvariant="normal">m</mi> </msub> </mrow> </semantics></math> abrupt changes to 1.5 <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi mathvariant="normal">m</mi> </msub> </mrow> </semantics></math> at 2 s. (<b>b</b>) Electromagnetic thrust response plot for <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi mathvariant="normal">m</mi> </msub> </mrow> </semantics></math> abrupt changes to 1.5 <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi mathvariant="normal">m</mi> </msub> </mrow> </semantics></math> at 2 s. (<b>c</b>) The three-phase current response plot for <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi mathvariant="normal">m</mi> </msub> </mrow> </semantics></math> abrupt changes to 1.5 <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi mathvariant="normal">m</mi> </msub> </mrow> </semantics></math> at 2 s. (<b>d</b>) Secondary flux linkage response plot for abrupt <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi mathvariant="normal">m</mi> </msub> </mrow> </semantics></math> change to 1.5 <math display="inline"><semantics> <mrow> <msub> <mi>L</mi> <mi mathvariant="normal">m</mi> </msub> </mrow> </semantics></math> at 2 s.</p>
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<p>Simulation results of improved MRAS speed estimation accelerated to 10 m/s. (<b>a</b>) Speed response plot for <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>s</mi> </msub> </mrow> </semantics></math> abrupt changes to 1.5 <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>s</mi> </msub> </mrow> </semantics></math> at 2 s. (<b>b</b>) Electromagnetic thrust response plot for <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>s</mi> </msub> </mrow> </semantics></math> abrupt changes to 1.5 <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>s</mi> </msub> </mrow> </semantics></math> at 2 s. (<b>c</b>) The three-phase current response plot for <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>s</mi> </msub> </mrow> </semantics></math> abrupt changes to 1.5 <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>s</mi> </msub> </mrow> </semantics></math> at 2 s. (<b>d</b>) Flux linkage Lissajous figure for <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>s</mi> </msub> </mrow> </semantics></math> abrupt changes to 1.5 <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>s</mi> </msub> </mrow> </semantics></math> at 2 s.</p>
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<p>Simulation results of speed and magnetizing inductance parameter identification based on improved interconnected MRAS observer. (<b>a</b>) Actual and identified values of magnetizing inductance. (<b>b</b>) Actual and identified speed values. (<b>c</b>) magnetized magnetizing inductance identification value. (<b>d</b>) Flux linkage Lissajous figure.</p>
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<p>Simulation results of speed and primary resistance parameter identification based on improved interconnected MRAS. (<b>a</b>) Actual and identified values of primary resistance. (<b>b</b>) Actual and identified speed values. (<b>c</b>) Flux linkage Lissajous figure. (<b>d</b>). Three-phase current.</p>
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<p>Comparison of speed and parameter identification results under <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>r</mi> </msub> </mrow> </semantics></math> variation. (<b>a</b>) Plot of <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi>r</mi> </msub> </mrow> </semantics></math> changes. (<b>b</b>) Actual and identified speed values. (<b>c</b>) Actual and identified values of primary resistance. (<b>d</b>). Actual and identified values of primary resistance.</p>
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<p>HIL test platform real-time simulation based on CPU-FPGA.</p>
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<p>Comparison diagram of velocity estimation system with current white noise. (<b>a</b>) Speed and speed error graphs. (<b>b</b>) Secondary flux linkage magnitude and electromagnetic thrust graphs.</p>
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<p>Experimental results under complex working conditions. (<b>a</b>) The speed and speed error of the improved interconnected MRAS observer. (<b>b</b>) The magnetizing inductance and identification error of the improved interconnected MRAS observer. (<b>c</b>) The primary resistance and identification error of the improved interconnected MRAS observer. (<b>d</b>) Three-phase current.</p>
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